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Resultant force on curved surface BCDEF

Short answer

Horizontal component, from pressure on vertical projection, is 625.8 kN; vertical component equals weight of water above surface up to equivalent free surface, 1812.2 kN. Resultant 1917 kN at 70.9° below horizontal.

Find the resultant pressure force due to water on a curved surface BCDEF of 10 m length as shown in figure below. [Figure: tank of water (s = 1) with gauge reading -19 kN/m² at the top; curved surface from B through C, D, E to F with portions of 2 m, 2 m, 2 m, 2 m, 3 m dimensions marked]

The resultant force on a curved surface has a horizontal component (force on the vertical projection) and a vertical component (weight of the liquid vertically above the surface up to the equivalent free surface). The figure is not fully readable, so the geometry below is assumed.

Assumed geometry (water on the concave side, length L=10L = 10 m, gauge at level of B reads −19-19 kN/m²):

   B |  gauge level, p = -19 kPa
     | BC = 2 m (vertical wall)
   C |
      \  CD, DE = two quarter circles,
       ) D  R = 2 m (semicircle C-D-E)
      /
   E |________ F   EF = 3 m (horizontal)

Vertical extent of B to E = 2 + 2 + 2 = 6 m, and EF lies at 6 m below B.

Pressure at B and equivalent free surface

pBγ=−199.81=−1.937 m\frac{p_B}{\gamma} = \frac{-19}{9.81} = -1.937\ \text{m}

The equivalent free surface is 1.937 m below B. Pressure at depth zz below B is p=−19+9.81zp = -19 + 9.81z kPa.

Horizontal component (vertical projection BE, height 6 m):

FH=L∫06(−19+9.81z) dz=L(−19×6+9.81×622)=10(−114+176.58)=625.8 kN\begin{aligned} F_H &= L\int_0^6 (-19 + 9.81z)\,dz = L\left(-19\times 6 + 9.81\times\frac{6^2}{2}\right)\\ &= 10(-114 + 176.58) = 625.8\ \text{kN} \end{aligned}

Vertical component

  • On the semicircle CDE: the upper quarter is pushed up and the lower quarter is pushed down by the liquid. The net force equals the weight of liquid in the half-disc enclosed between the two arcs:
FV1=γ(πR22)L=9.81×6.283×10=616.4 kN (downward)F_{V1} = \gamma\left(\frac{\pi R^2}{2}\right)L = 9.81\times 6.283\times 10 = 616.4\ \text{kN (downward)}
  • On the flat EF at 6 m depth: p=−19+9.81×6=39.86p = -19 + 9.81\times 6 = 39.86 kPa
FV2=39.86×3×10=1195.8 kN (downward)F_{V2} = 39.86\times 3\times 10 = 1195.8\ \text{kN (downward)} FV=616.4+1195.8=1812.2 kNF_V = 616.4 + 1195.8 = 1812.2\ \text{kN}

Resultant

F=625.82+1812.22=1917.2 kNθ=tan⁡−11812.2625.8=70.9∘ below the horizontal\begin{aligned} F &= \sqrt{625.8^2 + 1812.2^2} = 1917.2\ \text{kN}\\ \theta &= \tan^{-1}\frac{1812.2}{625.8} = 70.9^\circ \text{ below the horizontal} \end{aligned}

Answer: F≈1917F \approx 1917 kN (about 1.92 MN), inclined at 70.9∘70.9^\circ to the horizontal, with FH=625.8F_H = 625.8 kN and FV=1812.2F_V = 1812.2 kN. If the actual figure differs, use the same method: FH=∫p dAprojF_H = \int p\,dA_{proj} and FVF_V = weight of liquid up to the equivalent free surface.

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